Analyse complex circuits using Ohm's law, Kirchhoff's laws, and internal resistance — and apply these to solve problems involving series-parallel combinations, power and energy.
In a series circuit: same current everywhere; resistances add (R_total = R₁ + R₂ + …); voltages add up to the supply voltage.
In a parallel circuit: same voltage across each branch; currents add; 1/R_total = 1/R₁ + 1/R₂ + …
A real battery has an electromotive force (EMF) ε — the work done per unit charge by the battery — and an internal resistance r that opposes current inside the battery itself.
| Symbol | Quantity | Unit |
|---|---|---|
| ε | EMF (electromotive force) | Volt (V) |
| V_terminal | Terminal potential difference | Volt (V) |
| I | Current through battery | Ampere (A) |
| r | Internal resistance | Ohm (Ω) |
Kirchhoff's Current Law (KCL): At any junction (node) in a circuit, the sum of currents flowing in equals the sum of currents flowing out.
Kirchhoff's Voltage Law (KVL): The algebraic sum of all potential differences around any closed loop in a circuit equals zero.
The resistor with the highest resistance in a series circuit dissipates the most power (P = I²R, same I). In a parallel circuit, the resistor with the lowest resistance dissipates the most power (P = V²/R, same V).
Multi-loop circuits: Set up KVL equations for each independent loop. Choose a current direction for each loop (convention: clockwise). For each loop: Σ(EMF) = Σ(IR). Solve simultaneous equations.
Wheatstone Bridge: A circuit of four resistors in a diamond arrangement with a galvanometer across the middle. The bridge is balanced (galvanometer reads zero) when: R₁/R₂ = R₃/R₄. Used to measure unknown resistances precisely.
Maximum power transfer theorem: Maximum power is transferred from a source (with internal resistance r) to a load when the load resistance R_load = r (internal resistance). At this point, efficiency is 50%.
| Current I (A) | 0.5 | 1.0 | 1.5 | 2.0 |
|---|---|---|---|---|
| Terminal voltage V (V) | 8.5 | 7.0 | 5.5 | 4.0 |